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Spinon continuum in the Heisenberg quantum chain compound Sr2V3O9

Shang Gao1,2,3,*, Ling-Fang Lin4, Pontus Laurell4, Qiang Chen4, Qing Huang4, Clarina dela Cruz1, Krishnamurthy V. Vemuru1,5, Mark D. Lumsden1, Stephen E. Nagler1,4 et al.

Gonzalo Alvarez6, Elbio Dagotto2,4, Haidong Zhou4, Andrew D. Christianson2, and Matthew B. Stone1,†

  • 1Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 2Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 3Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China
  • 4Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA
  • 5BrainChip Inc., Laguna Hills, California 92653, USA
  • 6Computational Sciences & Engineering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA

  • *sgao.physics@gmail.com
  • †stonemb@ornl.gov

Phys. Rev. B 109, L020402 – Published 4 January, 2024

DOI: https://doi.org/10.1103/PhysRevB.109.L020402

Abstract

Magnetic excitations in the spin chain candidate Sr2V3O9 have been investigated by inelastic neutron scattering on a single crystal sample. A spinon continuum with a bandwidth of ∼22 meV is observed along the chain formed by alternating magnetic V4+ and nonmagnetic V5+ ions, which reveals the importance of the orbital degree of freedom in determining the chain axis as identified by prior electronic structure calculations. Incipient magnetic Bragg peaks due to weak ferromagnetic interchain couplings emerge when approaching the magnetic transition at TN∼5.3 K, while the excitations remain gapless within the instrumental resolution. Comparisons to the Bethe ansatz, density matrix renormalization group calculations, and effective field theories confirm Sr2V3O9 as a host of weakly coupled S=1/2 chains dominated by antiferromagnetic intrachain interactions of ∼7.1(1) meV.

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